TWI898845B - Light emitting element and manufacturing method thereof - Google Patents
Light emitting element and manufacturing method thereofInfo
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Abstract
Description
本發明涉及一種具有優異光效率的發光元件及其製造方法。 The present invention relates to a light-emitting element with excellent light efficiency and a method for manufacturing the same.
*本專利是在韓國政府(科學技術資訊通信部)的資助以及韓國研究基金會的支持下進行的研究成果(課題固有編號:1711195422,詳細課題編號:2022M3H4A3A01082883,課題名稱:突破外部量子效率30%的5μm級InGaN紅色微型LED核心技術開發)。 *This patent is the result of research conducted with funding from the Korean government (Ministry of Science and ICT) and support from the Korea Research Foundation (Project Number: 1711195422, Detailed Project Number: 2022M3H4A3A01082883, Project Title: Development of Core Technology for 5μm-Class InGaN Red Micro-LEDs with a Breakthrough External Quantum Efficiency of 30%).
*本專利申請根據美國專利法35U.S.C.119(a)要求於2023年7月25日提交的韓國專利申請第10-2023-0096662號、於2023年8月16日提交的韓國專利申請第10-2023-0106792號、於2023年9月25日提交的韓國專利申請第10-2023-0128003號及於2024年4月5日提交的韓國專利申請第10-2024-0046343號的優先權,其揭露內容透過引用整體併入本文。另外,本專利申請要求在其他國家提交的其他申請的優先權,其揭露內容也透過引用整體併入本文。 *This patent application claims priority under 35 U.S.C. 119(a) of the U.S. Patent Act to Korean Patent Application No. 10-2023-0096662, filed on July 25, 2023; Korean Patent Application No. 10-2023-0106792, filed on August 16, 2023; Korean Patent Application No. 10-2023-0128003, filed on September 25, 2023; and Korean Patent Application No. 10-2024-0046343, filed on April 5, 2024, the disclosures of which are hereby incorporated by reference in their entireties. Furthermore, this patent application claims priority to other applications filed in other countries, the disclosures of which are also hereby incorporated by reference in their entireties.
本部分中所描述的細節僅提供關於本實施例的背景資訊,而不構成現有技術。 The details described in this section merely provide background information about the present embodiment and do not constitute prior art.
發光二極體作為無機光源,被廣泛應用於顯示裝置、車用燈具及普通照明等各種領域。發光二極體具有壽命長、功耗低、回應速度快等優點,因此正在迅速取代現有光源。 LEDs, as inorganic light sources, are widely used in various fields, including display devices, automotive lighting, and general lighting. Due to their advantages such as long life, low power consumption, and fast response time, LEDs are rapidly replacing existing light sources.
發光二極體通常可以利用藍色、綠色及紅色的混合顏色來實現各種顏色。用於各種裝置的發光二極體包含多個像素,以實現各種圖像或顏色。每個像素包括藍色、綠色及紅色的子像素。這些子像素的組合決定相關像素的顏色,透過各個像素的組合實現圖像。 Light-emitting diodes (LEDs) can typically produce a variety of colors using a mixture of blue, green, and red. LEDs used in various devices contain multiple pixels to produce various images or colors. Each pixel consists of blue, green, and red sub-pixels. The combination of these sub-pixels determines the color of the associated pixel, and the combination of these sub-pixels creates an image.
現有的發光二極體通常是基於氮化物半導體製造的。與其他現有材料相比,基於氮化物半導體的發光二極體表現出相對優異的光效率。 Existing LEDs are typically manufactured based on nitride semiconductors. Compared to other existing materials, nitride semiconductor-based LEDs exhibit relatively superior light efficiency.
然而,現有的基於氮化物半導體的發光二極體在結構上存在以下問題。 However, existing nitride semiconductor-based LEDs have the following structural problems.
首先,基於氮化物半導體的發光二極體由於材料的晶格常數的差異而具有壓縮或膨脹的內部壓力。上述內部壓力(Strain,應變)在主動層內部產生壓電(Piezo)電場,並且所產生的壓電電場導致發光元件的內部發光效率顯著降低的問題。 First, nitride semiconductor-based LEDs experience internal pressure, either compression or expansion, due to differences in the material's lattice constant. This internal pressure (strain) generates a piezoelectric field within the active layer, significantly reducing the device's internal luminous efficiency.
另一個問題是由於透過p半導體層注入的電洞的密度和 遷移率顯著低於透過n半導體層注入的電子的密度和遷移率。因此,注入到主動層的電洞的數量相對顯著小於電子的數量,導致注入到主動層的多餘的電子積累在主動層和p半導體層之間的介面處。這些積累的電子產生另一個壓電電場,從而顯著降低電子和電洞結合產生光的概率。此外,隨著注入電流的增加,與電洞相比更多的電子聚集在主動層中,導致產生光的內量子效率逐漸下降。 Another problem arises because the density and mobility of holes injected through the p-semiconductor layer are significantly lower than those of electrons injected through the n-semiconductor layer. Therefore, the number of holes injected into the active layer is significantly smaller than the number of electrons. This causes excess electrons injected into the active layer to accumulate at the interface between the active layer and the p-semiconductor layer. These accumulated electrons generate another piezoelectric field, significantly reducing the probability of electron-hole combination to generate light. Furthermore, as the injected current increases, more electrons accumulate in the active layer compared to holes, causing the internal quantum efficiency of light generation to gradually decrease.
如上所述,由於上述晶格常數失配和電洞粒子和電子粒子之間的不平衡而產生內部壓力,透過所產生的內部壓力在主動層內部產生電場。電場擾亂注入的電洞粒子和電子粒子的流動並阻止它們的結合,導致減少光的產生概率的問題。 As mentioned above, the lattice constant mismatch and the imbalance between hole and electron particles generate internal pressure, which in turn generates an electric field within the active layer. This electric field disrupts the flow of injected hole and electron particles and prevents them from combining, resulting in a reduced probability of light generation.
本發明的一實施例的目的在於,提供一種發光元件及其製造方法,上述發光元件為了減少在主動層中由於電洞和電子之間的密度不平衡和晶格常數失配引起的內部壓力,透過調節晶格常數並提高電洞密度來提高光效率。 One embodiment of the present invention provides a light-emitting device and a method for manufacturing the same. The light-emitting device reduces internal stress in the active layer caused by density imbalance and lattice constant mismatch between holes and electrons, thereby improving light efficiency by adjusting the lattice constant and increasing the hole density.
本發明的一實施例的目的在於,提供一種發光元件及其製造方法,上述發光元件透過由不同材料實現的混合型包覆層來減少內部壓力的產生並提高電洞的密度,從而提高光效率。 One embodiment of the present invention provides a light-emitting device and a method for manufacturing the same. The light-emitting device utilizes a hybrid cladding layer made of different materials to reduce internal pressure and increase hole density, thereby improving light efficiency.
本發明的一實施例的目的在於,提供一種發光元件及其製造方法,上述發光元件透過具有如氧化鋅(ZnO)等的異種材料 的包覆層來減少內部壓力的產生並提高電洞的密度,從而提高光效率。 One embodiment of the present invention provides a light-emitting device and a method for manufacturing the same. The light-emitting device utilizes a cladding layer made of a different material, such as zinc oxide (ZnO), to reduce internal stress and increase hole density, thereby improving light efficiency.
本發明的一實施例的目的在於,提供一種發光元件及其製造方法,上述發光元件包括具有優異反射率的反射電極,因此具有優異的光輸出。 An embodiment of the present invention provides a light-emitting element and a method for manufacturing the same. The light-emitting element includes a reflective electrode having excellent reflectivity, thereby having excellent light output.
本發明的一實施例的目的在於,提供一種發光元件及其製造方法,上述發光元件透過使電流流動均勻並最小化由於電極對輸出光的干擾,從而改善光輸出。 An embodiment of the present invention provides a light-emitting device and a method for manufacturing the same, which improves light output by making the current flow uniform and minimizing interference with the output light caused by electrodes.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,並向上述主動層提供電洞;保護層,由在可見光波段的透光率和電導率分別等於或高於預設第一基準值和預設第二基準值的材料實現,並沉積在上述p型半導體層上,以保護上述p型半導體層免受外部影響;及電極,分別形成在上述n型包覆層和上述保護層上。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate, and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; and a p-type semiconductor layer, deposited on the active layer. and provides holes to the active layer; a protective layer, made of a material having a transmittance and conductivity in the visible light band equal to or greater than a preset first reference value and a preset second reference value, and deposited on the p-type semiconductor layer to protect the p-type semiconductor layer from external influences; and electrodes, respectively formed on the n-type cladding layer and the protective layer.
根據本發明的一個方面,提供一種發光元件的製造方法,其包括:沉積過程,在基板上依次沉積n型包覆層、主動層、p型半導體層及保護層;蝕刻過程,蝕刻n型包覆層、主動層、p型半導體層及保護層的一面積,並從上述保護層在垂直的方向上蝕刻 到上述n型包覆層的一部分;及形成過程,在上述保護層上形成第一電極,並在透過上述蝕刻過程暴露於外部的n型包覆層上形成第二電極。 According to one aspect of the present invention, a method for manufacturing a light-emitting device is provided, comprising: a deposition process of sequentially depositing an n-type cladding layer, an active layer, a p-type semiconductor layer, and a protective layer on a substrate; an etching process of etching a portion of the n-type cladding layer, the active layer, the p-type semiconductor layer, and the protective layer, and etching vertically from the protective layer to a portion of the n-type cladding layer; and a formation process of forming a first electrode on the protective layer and a second electrode on the portion of the n-type cladding layer exposed to the outside by the etching process.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型包覆層,由與上述n型包覆層不同的半導體材料實現,沉積在上述主動層上,並向上述主動層提供電洞;保護層,由在可見光波段的透光率和電導率分別等於或高於預設第一基準值和預設第二基準值的材料實現,並沉積在上述p型包覆層上,以保護上述p型包覆層免受外部影響;及電極,分別形成在上述n型包覆層和上述保護層上。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; and a p-type cladding layer, made of a semiconductor material different from that of the n-type cladding layer. A protective layer is deposited on the active layer and provides holes to the active layer; a protective layer is made of a material having a transmittance and conductivity in the visible light band equal to or higher than a preset first reference value and a preset second reference value, respectively, and is deposited on the p-type cladding layer to protect the p-type cladding layer from external influences; and electrodes are formed on the n-type cladding layer and the protective layer, respectively.
根據本發明的一個方面,提供一種發光元件的製造方法,其包括:沉積過程,在基板上依次沉積n型包覆層、主動層、p型包覆層及保護層;蝕刻過程,蝕刻n型包覆層、主動層、p型包覆層及保護層的一面積,並從上述保護層在垂直的方向上蝕刻到上述n型包覆層的一部分;及形成過程,在上述保護層上形成第一電極,並在透過上述蝕刻過程暴露於外部的n型包覆層上形成第二電極;上述p型包覆層由與n型包覆層不同的材料的半導體實現。 According to one aspect of the present invention, a method for manufacturing a light-emitting device is provided, comprising: a deposition process of sequentially depositing an n-type cladding layer, an active layer, a p-type cladding layer, and a protective layer on a substrate; an etching process of etching a portion of the n-type cladding layer, the active layer, the p-type cladding layer, and the protective layer, and etching vertically from the protective layer to a portion of the n-type cladding layer; and a formation process of forming a first electrode on the protective layer and a second electrode on the portion of the n-type cladding layer exposed to the outside by the etching process; the p-type cladding layer is formed of a semiconductor made of a different material from the n-type cladding layer.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導 體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,並向上述主動層提供電洞;第一電極,沉積在上述p型半導體層上,向p型半導體層供應電流,並將由上述主動層產生的光向上述n型包覆層方向反射;及第二電極,沉積在上述n型包覆層上,向n型包覆層供應電子,提高光提取效率。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, generating light by the combination of holes and electrons supplied from the n-type cladding layer; a p-type semiconductor layer, deposited on the active layer, supplying holes to the active layer; a first electrode, deposited on the p-type semiconductor layer, supplying current to the p-type semiconductor layer and reflecting light generated by the active layer toward the n-type cladding layer; and a second electrode, deposited on the n-type cladding layer, supplying electrons to the n-type cladding layer to improve light extraction efficiency.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,並向上述主動層提供電洞;第一電極,沉積在上述p型半導體層上,向p型半導體層供應電流,並將由上述主動層產生的光向上述n型包覆層方向反射;及第二電極,沉積在上述n型包覆層上,向n型包覆層供應電子,提高光提取效率;其中,上述第一電極和上述第二電極包括:金屬電極,在起到電極的作用的同時,反射入射到自身的光線;及保護層,沉積在上述金屬電極上,以保護上述金屬電極免受外部環境的影響。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate, and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; a p-type semiconductor layer, deposited on the active layer, and providing holes to the active layer; and a first electrode, deposited on the p-type semiconductor layer, and providing holes to the p-type semiconductor layer. The conductive layer supplies current and reflects light generated by the active layer toward the n-type cladding layer. The second electrode, deposited on the n-type cladding layer, supplies electrons to the n-type cladding layer, thereby improving light extraction efficiency. The first and second electrodes comprise metal electrodes that function as electrodes and reflect incident light, and protective layers deposited on the metal electrodes to protect them from the external environment.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,並向上述主動層提供電洞;第一電極,沉積在上述 p型半導體層上,向p型半導體層供應電流,並將由上述主動層產生的光向上述n型包覆層方向反射;及第二電極,沉積在上述n型包覆層上,向n型包覆層供應電子,提高光提取效率;其中,上述第一電極和上述第二電極包括:金屬電極,在起到電極的作用的同時,反射入射到自身的光線;保護層,沉積在上述金屬電極上,以保護上述金屬電極免受外部環境的影響;及金屬電極層,沉積在上述p型半導體層或上述n型包覆層與上述金屬電極之間,以提高上述金屬電極的接觸力。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons supplied from the n-type cladding layer meet and recombine to generate light; a p-type semiconductor layer, deposited on the active layer, and supplying holes to the active layer; and a first electrode, deposited on the p-type semiconductor layer, supplying a current to the p-type semiconductor layer and transmitting light generated by the active layer to the n-type semiconductor layer. The first electrode and the second electrode each comprise a metal electrode that reflects light incident on the p-type semiconductor layer or the n-type cladding layer; and a second electrode deposited on the p-type semiconductor layer or the n-type cladding layer to supply electrons to the n-type cladding layer, thereby improving light extraction efficiency. The first electrode and the second electrode each comprise a metal electrode that acts as an electrode and reflects light incident on the metal electrode; a protective layer deposited on the metal electrode to protect the metal electrode from the external environment; and a metal electrode layer deposited between the p-type semiconductor layer or the n-type cladding layer and the metal electrode to improve contact strength between the metal electrode and the p-type semiconductor layer.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,並向上述主動層提供電洞;第一電極,沉積在上述p型半導體層上,向p型半導體層供應電流,並將由上述主動層產生的光向上述n型包覆層方向反射;第二電極,沉積在上述n型包覆層上,向n型包覆層供應電子,提高光提取效率;及絕緣膜,層疊在上述n型包覆層、上述主動層及上述p型半導體層的側面以及上述第一電極和上述第二電極的側面和上面的一部分,以保護各構成免受外部影響。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate, and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; a p-type semiconductor layer, deposited on the active layer, and providing holes to the active layer; and a first electrode, deposited on the p-type semiconductor layer. The first electrode supplies current to the p-type semiconductor layer and reflects light generated by the active layer toward the n-type cladding layer. The second electrode is deposited on the n-type cladding layer and supplies electrons to the n-type cladding layer to improve light extraction efficiency. The insulating film is laminated on the side surfaces of the n-type cladding layer, the active layer, and the p-type semiconductor layer, as well as the side surfaces and a portion of the top surface of the first electrode and the second electrode to protect each component from external influences.
根據本發明的一個方面,提供一種發光元件的製造方法,其包括:蝕刻過程,利用在基板上具有依次由n型包覆層、主動層及p型半導體層構成的層結構的晶圓,進行蝕刻,將蝕刻進行到n 型包覆層的某一位置,以形成p-n接面的檯面結構;沉積過程,在檯面結構的上部表面上形成第一電極,並在透過上述蝕刻過程暴露於外部的n型包覆層上形成第二電極;及層疊過程,將絕緣膜層疊在上述n型包覆層、上述主動層及上述p型半導體層的側面以及上述第一電極和上述第二電極的側面和上面的一部分。 According to one aspect of the present invention, a method for manufacturing a light-emitting device is provided, comprising: an etching process, using a wafer having a layer structure composed of an n-type cladding layer, an active layer, and a p-type semiconductor layer on a substrate, etching to a certain position of the n-type cladding layer to form a p-n junction surface structure; a deposition process , forming a first electrode on the upper surface of the countertop structure, and forming a second electrode on the n-type cladding layer exposed to the outside by the etching process; and laminating an insulating film layer on the side surfaces of the n-type cladding layer, the active layer, and the p-type semiconductor layer, as well as the side surfaces and a portion of the top surface of the first electrode and the second electrode.
根據本發明的一個方面,在發光元件的製造方法中,與上述方法不同地,第一電極和第二電極可以透過不同的製程形成。即,提供一種發光元件的製造方法,其包括:第一沉積過程,在基板上依次形成的n型包覆層、主動層、p型半導體層及在p型半導體層中將形成p-n接面的檯面的特定區域的上部表面上沉積第一電極;蝕刻過程,進行蝕刻,將蝕刻進行到上述主動層、上述p型半導體層、上述第一電極及n型包覆層的某一位置,以形成檯面結構形狀;第二沉積過程,在透過上述蝕刻過程暴露於外部的n型包覆層上形成第二電極;及層疊過程,將絕緣膜層疊在上述n型包覆層、上述主動層及上述p型半導體層的側面以及上述第一電極和上述第二電極的側面和上面的一部分。 According to one aspect of the present invention, in a method for manufacturing a light-emitting element, unlike the above-mentioned method, the first electrode and the second electrode can be formed through different processes. That is, a method for manufacturing a light-emitting element is provided, which includes: a first deposition process, in which the first electrode is deposited on the upper surface of an n-type cladding layer, an active layer, a p-type semiconductor layer, and a specific region of the surface of the p-type semiconductor layer where a p-n junction will be formed, which is sequentially formed on a substrate; an etching process, in which the first electrode is deposited on the upper surface of the n-type cladding layer, the active layer, the p-type semiconductor layer, and the first electrode; and an etching process, in which the first electrode is deposited on the upper surface of the n-type cladding layer, the active layer, the p-type semiconductor layer, and the first electrode. A first electrode and a certain position of the n-type cladding layer are formed to form a countertop structure shape; a second deposition process is performed to form a second electrode on the n-type cladding layer exposed to the outside by the etching process; and a lamination process is performed to laminate an insulating film layer on the side surfaces of the n-type cladding layer, the active layer, and the p-type semiconductor layer, as well as the side surfaces and a portion of the top surface of the first electrode and the second electrode.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,向上述主動層提供電洞,但抑制或阻斷電洞向一部分區域供應;透明電極,沉積在上述p型半導體層上,向上述p型 半導體層供應電洞;第一電極,形成在上述透明電極上;及第二電極,沉積在上述n型包覆層上,向n型包覆層供應電子。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate, and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; and a p-type semiconductor layer, deposited on the substrate. A first electrode is formed on the transparent electrode; and a second electrode is deposited on the n-type cladding layer to supply electrons to the n-type cladding layer.
根據本發明的一方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,向上述主動層提供電洞,但抑制或阻斷電洞向一部分區域供應;透明電極,沉積在上述p型半導體層上,向上述p型半導體層供應電洞;第一電極,形成在上述透明電極上;及第二電極,沉積在上述n型包覆層上,並向n型包覆層供應電子;其中,上述p型半導體層包括:p型包覆層,由摻雜有p型摻雜劑的半導體材料實現,並沉積在上述主動層上,包含電流流動阻礙部,上述電流流動阻礙部阻斷電流,更具體地說,阻斷電洞流動;及p型氧化物層,由氧化鋅(ZnO)基化合物實現,沉積在上述p型包覆層上。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate, and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; a p-type semiconductor layer, deposited on the active layer, and providing holes to the active layer but suppressing or blocking the supply of holes to a certain region; and a transparent electrode, deposited on the p-type semiconductor layer, and providing light to the p-type semiconductor layer. supplying holes; a first electrode formed on the transparent electrode; and a second electrode deposited on the n-type cladding layer and supplying electrons to the n-type cladding layer. The p-type semiconductor layer comprises: a p-type cladding layer made of a semiconductor material doped with a p-type dopant, deposited on the active layer, and comprising a current flow barrier, wherein the current flow barrier blocks current, more specifically, blocks the flow of holes; and a p-type oxide layer made of a zinc oxide (ZnO)-based compound, deposited on the p-type cladding layer.
根據本發明的一個方面,提供一種發光元件,其包括:基板;n型包覆層,沉積在上述基板上,由摻雜有n型摻雜劑的半導體材料實現;主動層,沉積在上述n型包覆層上,電洞和從n型包覆層提供的電子相遇並複合,以產生光;p型半導體層,沉積在上述主動層上,向上述主動層提供電洞,但抑制或阻斷電洞向一部分區域供應;透明電極,沉積在上述p型半導體層上,向上述p型半導體層供應電洞;第一電極,形成在上述透明電極上;及第二電極,沉積在上述n型包覆層上,並向n型包覆層供應電子;其中, 上述p型半導體層包括:p型包覆層,由摻雜有p型摻雜劑的半導體材料實現,並沉積在上述主動層上,包含電流流動阻礙部和漏電流防止部,上述電流流動阻礙部阻斷電流或電洞流動,上述漏電流防止部阻斷漏電流產生;及p型氧化物層,由氧化鋅(ZnO)基化合物實現,沉積在上述p型包覆層上。 According to one aspect of the present invention, a light-emitting element is provided, comprising: a substrate; an n-type cladding layer, deposited on the substrate and made of a semiconductor material doped with an n-type dopant; an active layer, deposited on the n-type cladding layer, wherein holes and electrons provided from the n-type cladding layer meet and recombine to generate light; a p-type semiconductor layer, deposited on the active layer, which provides holes to the active layer but suppresses or blocks the supply of holes to a certain region; a transparent electrode, deposited on the p-type semiconductor layer, which supplies holes to the p-type semiconductor layer; a first electrode; The p-type semiconductor layer comprises a first electrode formed on the transparent electrode; a second electrode deposited on the n-type cladding layer and supplying electrons to the n-type cladding layer; wherein the p-type semiconductor layer comprises: a p-type cladding layer made of a semiconductor material doped with a p-type dopant and deposited on the active layer, comprising a current flow blocking portion and a leakage current preventing portion, the current flow blocking portion blocking the flow of current or holes, and the leakage current preventing portion preventing the generation of leakage current; and a p-type oxide layer made of a zinc oxide (ZnO)-based compound and deposited on the p-type cladding layer.
根據本發明的一個方面,提供一種發光元件的製造方法,其包括:第一沉積過程,在基板上依次沉積n型包覆層、主動層及p型包覆層;處理過程,對在上述p型包覆層內的預設區域進行使用氧或含氧氣體的等離子體處理或離子/電子注入(Implantation)製程;第二沉積過程,在上述p型包覆層上沉積p型氧化物層和透明電極;蝕刻過程,從上述透明電極將蝕刻進行到上述n型包覆層的某一位置,以形成檯面結構形狀;及金屬電極形成過程,在上述透明電極上形成第一電極,在暴露於外部的n型包覆層上形成第二電極。 According to one aspect of the present invention, a method for manufacturing a light-emitting element is provided, comprising: a first deposition process of sequentially depositing an n-type cladding layer, an active layer, and a p-type cladding layer on a substrate; a treatment process of plasma treatment or ion/electron implantation using oxygen or an oxygen-containing gas in a predetermined region within the p-type cladding layer; a second deposition process of depositing a p-type oxide layer and a transparent electrode on the p-type cladding layer; an etching process of etching from the transparent electrode to a certain position within the n-type cladding layer to form a countertop structure; and a metal electrode formation process of forming a first electrode on the transparent electrode and a second electrode on the exposed portion of the n-type cladding layer.
根據本發明的一方面,提供一種發光元件的製造方法,其包括:第一沉積過程,在基板上依次沉積n型包覆層、主動層及p型包覆層;第一處理過程,對在上述p型包覆層內的預設區域進行使用氧或含氧氣體的等離子體處理或離子/電子注入製程;第二沉積過程,在上述p型包覆層上沉積p型氧化物層和透明電極;蝕刻過程,從上述透明電極將蝕刻進行到上述n型包覆層的某一位置,以形成檯面結構形狀;第二處理過程,進行使用氧或含氧氣體的等離子體處理;及形成過程,在上述透明電極上形成第一電 極,在暴露於外部的n型包覆層上形成第二電極。 According to one aspect of the present invention, a method for manufacturing a light-emitting element is provided, comprising: a first deposition process, in which an n-type cladding layer, an active layer, and a p-type cladding layer are sequentially deposited on a substrate; a first treatment process, in which a predetermined area within the p-type cladding layer is subjected to a plasma treatment or an ion/electron implantation process using oxygen or an oxygen-containing gas; a second deposition process, in which an active layer is deposited on a predetermined area within the p-type cladding layer; A p-type oxide layer and a transparent electrode are deposited on the first layer; an etching process is performed from the transparent electrode to a certain position on the n-type cladding layer to form a countertop structure; a second treatment process is performed using a plasma treatment using oxygen or an oxygen-containing gas; and a formation process is performed to form a first electrode on the transparent electrode and a second electrode on the exposed portion of the n-type cladding layer.
如上所述,根據本發明的一個方面,存在如下優點,即,減少內部壓力的產生並提高電洞密度,從而能夠提高光效率。 As described above, according to one aspect of the present invention, there is an advantage in that the generation of internal pressure is reduced and the hole density is increased, thereby being able to improve light efficiency.
根據本發明的一個方面,存在如下優點,即,透過具有由不同材料的半導體材料實現的混合型包覆層來減少內部壓力的產生並提高電洞密度,從而能夠提高光效率。 According to one aspect of the present invention, a hybrid cladding layer made of different semiconductor materials can reduce internal stress and increase hole density, thereby improving light efficiency.
根據本發明的一個方面,存在如下優點,即,透過具有如氧化鋅(ZnO)等的異種材料的包覆層來減少內部壓力的產生並提高電洞的密度,從而能夠提高光效率。 According to one aspect of the present invention, there is an advantage in that the generation of internal pressure is reduced and the density of holes is increased by using a cladding layer made of a different material such as zinc oxide (ZnO), thereby improving light efficiency.
根據本發明的一個方面,存在如下優點,即,透過使電流流動均勻且包括具有優異反射率的反射電極來能夠具有優異的光輸出。 According to one aspect of the present invention, there is an advantage in that excellent light output can be achieved by making the current flow uniform and including a reflective electrode with excellent reflectivity.
另外,根據本發明的一個方面,存在如下優點,即,透過最小化由於不透明金屬電極造成的對光輸出的阻礙,從而能夠提高光輸出。 In addition, according to one aspect of the present invention, there is an advantage in that light output can be improved by minimizing the obstruction of light output caused by the opaque metal electrode.
100、1100、1900、2700、3800:發光元件 100, 1100, 1900, 2700, 3800: Light-emitting element
110、2710:基板 110, 2710: Substrate
1110、130、2730:主動層 1110, 130, 2730: Active layer
1120、210、2810:p型包覆層 1120, 210, 2810: p-type cladding layer
120、2720:n型包覆層 120, 2720: n-type cladding layer
1210:第一阻擋層 1210: First barrier layer
1220、1220a、1220b、1220c、1220n:井層 1220, 1220a, 1220b, 1220c, 1220n: Well layers
1230:第二阻擋層 1230: Second barrier layer
1310a、1310b、1310c、1310n:阻擋層 1310a, 1310b, 1310c, 1310n: Barrier layer
140、2740:p型半導體層 140, 2740: p-type semiconductor layer
1410、220:內部壓力緩解層 1410, 220: Internal pressure relief layer
1420、230:電洞傳輸率提高層 1420, 230: Hole transport efficiency enhancement layer
150:電極、保護層 150: Electrode, protective layer
155、160、165、2760、2765:電極 155, 160, 165, 2760, 2765: Electrodes
1910:絕緣膜 1910: Insulation Film
2010:金屬電極 2010: Metal Electrode
2020:保護層 2020: Protective layer
2030:金屬接觸層 2030: Metal contact layer
2750:透明電極 2750: Transparent Electrode
2820:p型氧化物層 2820: p-type oxide layer
2830:電流流動阻礙部 2830: Current flow resistance
3810:漏電流防止部 3810: Leakage current prevention unit
圖1為示出根據本發明的第一實施例的發光元件的構成的圖。 FIG1 is a diagram showing the structure of a light-emitting element according to the first embodiment of the present invention.
圖2為示出根據本發明的第一實施例的p型半導體層的構成的圖。 FIG2 is a diagram showing the structure of a p-type semiconductor layer according to the first embodiment of the present invention.
圖3為示出根據本發明的第一實施例的發光元件和現有發光元件的內量子效率的圖表。 FIG3 is a graph showing the internal quantum efficiency of the light-emitting element according to the first embodiment of the present invention and a conventional light-emitting element.
圖4為比較根據本發明的第一實施例的發光元件和現有發光元件的主動層的內部特性的圖。 FIG4 is a graph comparing the internal characteristics of the active layer of the light-emitting element according to the first embodiment of the present invention and a conventional light-emitting element.
圖5至圖10為示出根據本發明的第一實施例的發光元件的製造過程的圖。 Figures 5 to 10 are diagrams illustrating the manufacturing process of the light-emitting element according to the first embodiment of the present invention.
圖11為示出根據本發明的第二實施例的發光元件的構成的圖。 FIG11 is a diagram showing the structure of a light-emitting element according to a second embodiment of the present invention.
圖12和圖13為示出根據本發明的第二實施例的主動層的構成和能帶特性的圖。 Figures 12 and 13 are diagrams showing the structure and energy band characteristics of the active layer according to the second embodiment of the present invention.
圖14為示出根據本發明的第二實施例的p型包覆層的構成的圖。 FIG14 is a diagram showing the structure of a p-type cladding layer according to the second embodiment of the present invention.
圖15至圖17為示出根據本發明的第二實施例的發光元件的製造過程的圖。 Figures 15 to 17 are diagrams illustrating the manufacturing process of a light-emitting element according to the second embodiment of the present invention.
圖18為示出根據本發明的第二實施例的發光元件的根據施加電流的發光強度變化的圖。 FIG18 is a graph showing changes in the light-emitting intensity of a light-emitting element according to the second embodiment of the present invention depending on the applied current.
圖19為示出根據本發明的第三實施例的發光元件的構成的圖。 FIG19 is a diagram showing the structure of a light-emitting element according to a third embodiment of the present invention.
圖20a及圖20b為示出根據本發明的第三實施例的電極層的構成的圖。 Figures 20a and 20b are diagrams showing the structure of an electrode layer according to the third embodiment of the present invention.
圖21為示出由不同成分實現的電極的電壓和電流特性的圖表。 Figure 21 is a graph showing the voltage and current characteristics of electrodes realized with different compositions.
圖22a及圖22b為示出Al或Al/Ag基歐姆電極的電壓和電流特性的圖表。 Figures 22a and 22b are graphs showing the voltage and current characteristics of Al or Al/Ag-based ohmic electrodes.
圖23和圖24為示出根據本發明的第三實施例的電極的結構的圖。 Figures 23 and 24 are diagrams showing the structure of an electrode according to a third embodiment of the present invention.
圖25和圖26為示出根據本發明的第三實施例的發光元件的製造過程的圖。 Figures 25 and 26 are diagrams illustrating the manufacturing process of a light-emitting element according to the third embodiment of the present invention.
圖27為示出根據本發明的第四實施例的發光元件的構成的圖。 FIG27 is a diagram showing the structure of a light-emitting element according to a fourth embodiment of the present invention.
圖28為示出根據本發明的第四或第五實施例的p型半導體層的構成的圖。 FIG28 is a diagram showing the structure of a p-type semiconductor layer according to the fourth or fifth embodiment of the present invention.
圖29為根據本發明的第四或第五實施例的p型半導體層的平面圖。 Figure 29 is a plan view of a p-type semiconductor layer according to the fourth or fifth embodiment of the present invention.
圖30為比較根據本發明的第四實施例的發光元件和現有發光元件的光效率的圖。 FIG30 is a graph comparing the light efficiencies of the light emitting element according to the fourth embodiment of the present invention and conventional light emitting elements.
圖31至圖37為示出根據本發明的一實施例的發光元件的製造過程的圖。 Figures 31 to 37 are diagrams illustrating a manufacturing process of a light-emitting element according to an embodiment of the present invention.
圖38為示出根據本發明的第五實施例的發光元件的構成的圖。 FIG38 is a diagram showing the structure of a light-emitting element according to a fifth embodiment of the present invention.
本發明能夠實施多種變更且能夠具有各種實施例,因而要在圖中例示特定實施例並詳細地進行說明。但這並不是要將本 發明限定於特定的實施方式,而應當理解為包括落入本發明的思想以及技術範圍的所有變更、等同物乃至替代物。在說明每個圖時,相似的附圖標記用於相似的結構要素。 The present invention is susceptible to numerous modifications and various embodiments, and thus specific embodiments are illustrated in the drawings and described in detail. However, this is not intended to limit the present invention to any specific embodiment; rather, the present invention should be understood to encompass all modifications, equivalents, and even alternatives falling within the spirit and technical scope of the present invention. Similar reference numerals are used to represent similar structural elements in each figure.
“第一”、“第二”、“A”、“B”等的術語可用於說明各種結構要素,但上述結構要素並不限定於該術語。上述術語用來將一個結構要素與另一個結構要素區分開。例如,在不脫離本發明的保護範圍的前提下,“第一結構要素”可以被稱為“第二結構要素”,類似地,第二結構要素”還可以被稱為“第一結構要素”。術語“和/或”可包括多個相關描述專案的組合或多個相關描述專案中的任意一個。 Terms such as "first," "second," "A," and "B" may be used to describe various structural elements, but the structural elements described above are not limited to these terms. These terms are used to distinguish one structural element from another. For example, without departing from the scope of protection of the present invention, a "first structural element" can be referred to as a "second structural element," and similarly, a "second structural element" can be referred to as a "first structural element." The term "and/or" may include a combination of multiple related described items or any one of the multiple related described items.
將理解的是,當元件被稱為“連接”或“結合”到另一結構要素時,兩個結構要素可彼此直接連接或結合,或者在兩個結構要素之間可存在中間結構要素。相反,當某個結構要素被稱為“直接連接或結合”時,在兩個結構要素之間不存在中間結構要素。 It will be understood that when an element is referred to as being “connected” or “coupled” to another structural element, the two structural elements may be directly connected or coupled to each other, or an intervening structural element may exist between the two structural elements. In contrast, when a structural element is referred to as being “directly connected or coupled,” there are no intervening structural elements between the two structural elements.
在本申請中使用的術語只是為了說明特定實施例而使用的,並非要限定本發明。只要在文中未明確地區別說明,表示單數的說明應當理解為包括複數。在本申請中,如“包括(包含)”或“具有”等的術語指示陳述的特徵、數位、步驟、操作、結構要素、部件或它們的組合的存在,但不排除存在或添加一個或更多個其他特徵、數位、步驟、操作、結構要素、部件或它們的組合。 The terms used in this application are intended only to describe specific embodiments and are not intended to limit the present invention. Unless otherwise specified, terms indicating the singular should be understood to include the plural. In this application, terms such as "including," "comprising," or "having" indicate the presence of stated features, numbers, steps, operations, structural elements, components, or combinations thereof, but do not preclude the presence or addition of one or more other features, numbers, steps, operations, structural elements, components, or combinations thereof.
除非另有定義,包括技術或科學術語其它這裡使用的所 有術語具有本發明所屬領域的一般技術人員通常所理解的相同含義。 Unless otherwise defined, all terms used herein, including technical or scientific terms, have the same meaning as commonly understood by a person of ordinary skill in the art to which this invention belongs.
與通常使用的詞典中的定義相同的術語,應當解釋為與有關技術的文章中的意義一致,並且,若在本說明中沒有明確定義,則不能解釋為具有異常或過於形式的意義。 Terms that have the same meaning as those defined in commonly used dictionaries should be interpreted as having the same meaning as in the relevant technical articles and should not be interpreted as having unusual or overly formal meanings unless expressly defined in this specification.
另外,本發明的每個實施例中包括的每個配置、過程、製程或方法可以在技術上彼此不矛盾的範圍內共用。 In addition, each configuration, process, process, or method included in each embodiment of the present invention can be shared within the scope of technical non-inconsistency.
圖1為示出根據本發明的一實施例的發光元件的構成的圖。 FIG1 is a diagram showing the structure of a light-emitting element according to an embodiment of the present invention.
參照圖1,根據本發明的一實施例的發光元件100包括基板110、n型包覆層120、主動層130、p型半導體層140、保護層150及電極160、165。 1 , a light-emitting device 100 according to one embodiment of the present invention includes a substrate 110, an n-type cladding layer 120, an active layer 130, a p-type semiconductor layer 140, a protective layer 150, and electrodes 160 and 165.
基板110在其上端生長n型包覆層120。基板110可以由藍寶石實現,但不一定限於此,而可以用能夠生長氮化鎵(GaN)的任何材料來代替。 The n-type cladding layer 120 is grown on the upper end of the substrate 110. The substrate 110 can be made of sapphire, but is not necessarily limited thereto and can be replaced by any material capable of growing gallium nitride (GaN).
n型包覆層120沉積在基板110上,且由摻雜有n型摻雜劑的半導體材料實現,以向主動層130提供電子。可以透過外延單晶(Epitaxy Single Crystal)沉積方法將n型包覆層120沉積在基板110上。n型包覆層120可以由n型氮化鎵(n-GaN)實現,但不一定限於此,而可以用n型InGaN、n型AlGaN或n型AlInGaN或其組合來代替。 The n-type cladding layer 120 is deposited on the substrate 110 and is made of a semiconductor material doped with an n-type dopant to provide electrons to the active layer 130. The n-type cladding layer 120 can be deposited on the substrate 110 using an epitaxy single crystal deposition method. The n-type cladding layer 120 can be made of, but is not limited to, n-type gallium nitride (n-GaN) and can be substituted with n-type InGaN, n-type AlGaN, n-type AlInGaN, or a combination thereof.
主動層130沉積在n型包覆層120上。在主動層130中, 從n型包覆層120提供的電子和從p型半導體層140提供的電洞相遇並複合,以產生光。主動層130由具有相對小的能帶隙的井層(圖中未示出)和具有相對大的能帶隙的阻擋層(圖中未示出)實現。主動層130可以由具有不同In濃度的InGaN層、InGaN/GaN或GaN/AlGaN層或它們的組合實現。 Active layer 130 is deposited on n-type cladding layer 120. In active layer 130, electrons supplied from n-type cladding layer 120 and holes supplied from p-type semiconductor layer 140 meet and recombine, generating light. Active layer 130 is implemented by a well layer (not shown) with a relatively small energy bandgap and a barrier layer (not shown) with a relatively large energy bandgap. Active layer 130 can be implemented by InGaN layers with varying In concentrations, InGaN/GaN, GaN/AlGaN layers, or combinations thereof.
p型半導體層140沉積在主動層130上並向主動層130提供電洞。此時,由於p型半導體層140被實現為具有圖2所示的結構,因此可以在最小化內部壓力(應變)的同時提高向主動層130的電洞的傳輸率。 P-type semiconductor layer 140 is deposited on active layer 130 and provides holes to active layer 130. Since p-type semiconductor layer 140 has the structure shown in FIG2 , it is possible to improve the transfer rate of holes to active layer 130 while minimizing internal stress (strain).
圖2為示出根據本發明的一實施例的p型半導體層的構成的圖,圖4為比較根據本發明的一實施例的發光元件和現有發光元件的主動層的內部特性的圖。 Figure 2 shows the structure of a p-type semiconductor layer according to an embodiment of the present invention, and Figure 4 compares the internal characteristics of the active layer of a light-emitting element according to an embodiment of the present invention and a conventional light-emitting element.
參照圖2,根據本發明的一實施例的p型半導體層140包括p型包覆層210、內部壓力緩解層220及電洞傳輸率提高層230。 2 , the p-type semiconductor layer 140 according to one embodiment of the present invention includes a p-type cladding layer 210 , an internal stress relief layer 220 , and a hole transport efficiency enhancement layer 230 .
p型包覆層210沉積在主動層130的正上端,由摻雜有p型摻雜劑的半導體材料實現,以向主動層130提供傳輸的電洞。可以透過外延單晶沉積方法將p型包覆層210沉積在主動層130上。與現有技術相同地,p型包覆層210可以由p型氮化鎵(p-GaN)實現,但不一定限於此,而可以用p型InGaN、p型AlGaN或p型AlInGaN或其組合來代替。 A p-type cladding layer 210 is deposited directly above the active layer 130. It is made of a semiconductor material doped with a p-type dopant to provide holes for transmission to the active layer 130. The p-type cladding layer 210 can be deposited on the active layer 130 using an epitaxial single crystal deposition method. As with conventional techniques, the p-type cladding layer 210 can be made of p-type gallium nitride (p-GaN), but is not necessarily limited to this material. Alternatively, p-type InGaN, p-type AlGaN, p-type AlInGaN, or a combination thereof can be used.
內部壓力緩解層220以預設厚度沉積在p型包覆層210上,以使主動層130和p型包覆層210之間可能出現的內部壓力 最小化。 The internal stress relief layer 220 is deposited on the p-type cladding layer 210 to a predetermined thickness to minimize any internal stress that may occur between the active layer 130 and the p-type cladding layer 210.
內部壓力緩解層220可以透過化學氣相沉積(CVD:Chemical Vapor Deposition)、分子束晶體生長(MBE:Molecular Beam Epitaxy)、脈衝鐳射沉積(PLD:Pulsed Laser Deposition)或各種沉積方法的混合方法(HBD:Hybrid Beam Deposition,混合束沉積)進行沉積。尤其,為了解決上述的問題,內部壓力緩解層220由氧化鋅基化合物(下面將描述)實現,因此,優選使用利用專用於氧化物沉積的設備開發的HBD方法來沉積。 The internal stress relief layer 220 can be deposited using chemical vapor deposition (CVD), molecular beam epitaxy (MBE), pulsed laser deposition (PLD), or a hybrid method (HBD) of these deposition methods. In particular, to address the aforementioned issues, the internal stress relief layer 220 is preferably formed from a zinc oxide-based compound (described below). Therefore, it is preferably deposited using the HBD method, which utilizes equipment specifically developed for oxide deposition.
內部壓力緩解層220由氧化鋅(ZnO)基化合物實現。內部壓力緩解層220可以由具有六方晶體結構的氧化鋅(ZnO)實現,或由包含鋅(Zn)和在元素週期表中的第2族和第6族的元素的氧化物實現。例如,內部壓力緩解層220可以由ZnO、BeZnO、MgZnO、BeMgZnO、ZnSO、ZnSeO、ZnSSeO、ZnCdO或ZnCdSeO實現。以這種方式實現的內部壓力緩解層220具有與p型包覆層210非常相似的物理特性、電學特性及光學特性,但具有比p型包覆層210更大的晶格常數和更高的電洞濃度。內部壓力緩解層220可以降低存在於主動層130和p型包覆層210之間的內部壓力。當存在於主動層130和p型包覆層210之間的內部壓力減小時,可以發生如圖4所示的效果。參照圖4,可以確認,與現有的LED相比,發光元件100具有相對較小的平帶電壓(Flat Band Voltage)和壓電電壓,因此具有相對較寬的耗盡(Depletion)層寬度。因此,向主動層130注入電洞變得更容易,且可以顯著提高內量子效率。 The internal stress relief layer 220 is implemented by a zinc oxide (ZnO)-based compound. The internal stress relief layer 220 may be implemented by zinc oxide (ZnO) having a hexagonal crystal structure, or by an oxide containing zinc (Zn) and elements from Groups 2 and 6 of the periodic table. For example, the internal stress relief layer 220 may be implemented by ZnO, BeZnO, MgZnO, BeMgZnO, ZnSO, ZnSeO, ZnSSeO, ZnCdO, or ZnCdSeO. The internal stress relief layer 220 implemented in this manner has physical, electrical, and optical properties very similar to those of the p-type cladding layer 210, but has a larger lattice constant and a higher hole concentration than the p-type cladding layer 210. The internal stress relief layer 220 can reduce the internal stress between the active layer 130 and the p-type cladding layer 210. When the internal stress between the active layer 130 and the p-type cladding layer 210 is reduced, the effect shown in FIG. 4 can occur. Referring to Figure 4 , it can be seen that compared to conventional LEDs, light-emitting element 100 has a relatively small flat-band voltage and piezoelectric voltage, resulting in a relatively wide depletion layer. This facilitates hole injection into active layer 130 and significantly improves internal quantum efficiency.
內部壓力緩解層220可以在p型包覆層210上沉積至預設厚度。在此,預設厚度可以是10nm至1000nm,更優選地,可以是50nm至200nm。 The internal stress relief layer 220 can be deposited on the p-type cladding layer 210 to a predetermined thickness. Here, the predetermined thickness can be 10 nm to 1000 nm, more preferably 50 nm to 200 nm.
為了將更多的電洞注入到主動層130中,內部壓力緩解層220可以以預設濃度摻雜有p型雜質,或者可以在不摻雜雜質的情況下產生鋅空位。 To inject more holes into the active layer 130, the internal stress relief layer 220 can be doped with p-type impurities at a preset concentration, or zinc vacancies can be generated without doping.
內部壓力緩解層220可以摻雜有在預設濃度範圍內的p型雜質。摻雜的雜質可以是p型受體(Acceptor)雜質,例如,可以是H、Li、Na、K、Rb、Cs、Fr、Cu、Ag、N、P、As、Sb及Bi中的一種以上。這些p型受體雜質可以摻雜到氧化鋅基化合物中以形成內部壓力緩解層220,且可以以預設濃度摻雜。預設濃度為1*1017原子/cm-3至1*1020原子/cm-3,更優選地,可以是5*1018原子/cm-3至5*1019原子/cm-3。 Internal stress relief layer 220 may be doped with p-type impurities within a preset concentration range. The doped impurities may be p-type acceptor impurities, such as one or more of H, Li, Na, K, Rb, Cs, Fr, Cu, Ag, N, P, As, Sb, and Bi. These p-type acceptor impurities may be doped into a zinc oxide-based compound to form internal stress relief layer 220, and may be doped at a preset concentration. The preset concentration is 1*10 17 atoms/cm -3 to 1*10 20 atoms/cm -3 , and more preferably 5*10 18 atoms/cm -3 to 5*10 19 atoms/cm -3 .
另一方面,內部壓力緩解層220可以在不摻雜雜質的情況下產生鋅空位。內部壓力緩解層220可以透過在p型包覆層210的表面上沉積未摻雜的氧化鋅基化合物、然後在含氧環境中對其進行熱處理來形成。熱處理可以在相應的環境中在400℃至700℃的溫度、更優選地,在450℃至550℃的溫度下進行1分鐘至600分鐘、甚至更優選進行10分鐘至60分鐘。當在上述環境中對氧化鋅基化合物進行熱處理時,發生構成氧化鋅基化合物的金屬原子,例如,鋅的含量變得不足的現象,從而內部壓力緩解層220的電洞濃度可以提高。內部壓力緩解層220可以經過上述過程,最 小化在主動層130和p型包覆層210之間可能出現的內部壓力,且使電洞更容易注入到主動層130中。 On the other hand, the internal stress relief layer 220 can generate zinc vacancies without doping. The internal stress relief layer 220 can be formed by depositing an undoped zinc oxide-based compound on the surface of the p-type cladding layer 210 and then heat-treating the compound in an oxygen-containing environment. The heat treatment can be performed in a suitable environment at a temperature of 400°C to 700°C, more preferably 450°C to 550°C, for 1 minute to 600 minutes, and even more preferably 10 minutes to 60 minutes. When the zinc oxide-based compound is heat-treated in the aforementioned environment, the content of metal atoms, such as zinc, that constitute the zinc oxide-based compound becomes insufficient, thereby increasing the hole concentration in the internal stress relief layer 220. Through this process, the internal stress relief layer 220 minimizes the internal stress that may occur between the active layer 130 and the p-type cladding layer 210 and facilitates hole injection into the active layer 130.
電洞傳輸率提高層230以預設厚度沉積在內部壓力緩解層220上,以形成歐姆接觸,以便在內部壓力緩解層220和保護層150之間形成低接觸電阻。 The hole transport efficiency enhancement layer 230 is deposited on the internal stress relief layer 220 with a predetermined thickness to form an ohmic contact, thereby creating a low contact resistance between the internal stress relief layer 220 and the protective layer 150.
與內部壓力緩解層220同樣地,電洞傳輸率提高層230也由氧化鋅(ZnO)基化合物實現,且以預設厚度沉積。P型雜質、n型雜質或p型/n型雜質可以摻雜到電洞傳輸率提高層230中。電洞傳輸率提高層230可以透過基於快速熱處理製程、等離子體處理/離子注入製程或使用酸或鹼溶液的製程摻雜雜質來實現。為了保證主動層130中產生的光子不被自身吸收且電流能夠透過隧道效應等而容易流動,預設厚度可以是50nm以下,更優選在1nm至10nm的範圍內。 Similar to the internal stress relief layer 220, the hole transport enhancing layer 230 is also made of a zinc oxide (ZnO)-based compound and deposited to a predetermined thickness. P-type impurities, n-type impurities, or both p-type and n-type impurities can be doped into the hole transport enhancing layer 230. The hole transport enhancing layer 230 can be doped using a rapid thermal process, plasma treatment/ion implantation, or a process using an acid or alkaline solution. To ensure that photons generated in the active layer 130 are not absorbed by itself and that current can flow easily through tunneling effects, the predetermined thickness can be less than 50 nm, more preferably within a range of 1 nm to 10 nm.
電洞傳輸率提高層230以預設濃度摻雜有雜質。在此,預設濃度可以是改變能帶隙以使內部壓力緩解層220與保護層150之間形成歐姆接觸的程度的濃度,其可以是1*1019原子/cm-3以上,更具體地,可以是5*1019原子/cm-3至1*1021原子/cm-3。摻雜到電洞傳輸率提高層230的雜質作為受體雜質,例如,可以是H、Li、Na、K、Rb、Cs、Fr、Cu、Ag、N、P、As、Sb及Bi中的一種以上。更優選地,受體雜質可以是N、P或As,更優選地,可以是N或As。另一方面,摻雜到電洞傳輸率提高層230中的雜質是施體(Donor)雜質,而可以是B、Al、Ga、In、Ti、F、Cl、 Br及I中的一種以上。更優選地,施體雜質可以是Al、Ga或In。或者,摻雜到電洞傳輸率提高層230中的雜質可以包括一種以上的受體雜質和一種以上的施體雜質。這些雜質以等於或大於預設濃度的濃度摻雜到電洞傳輸率提高層230中。 The hole transport enhancing layer 230 is doped with an impurity at a predetermined concentration. The predetermined concentration may be a concentration sufficient to alter the energy band gap and form ohmic contact between the internal stress relief layer 220 and the protective layer 150. The predetermined concentration may be greater than 1*10 19 atoms/cm -3 , and more specifically, may be between 5*10 19 atoms/cm -3 and 1*10 21 atoms/cm -3 . The impurity doped into the hole transport enhancing layer 230 serves as an acceptor impurity and may be, for example, one or more of H, Li, Na, K, Rb, Cs, Fr, Cu, Ag, N, P, As, Sb, and Bi. More preferably, the acceptor impurity may be N, P, or As, and even more preferably, N or As. On the other hand, the impurities doped into the hole transport enhancing layer 230 are donor impurities and may be one or more of B, Al, Ga, In, Ti, F, Cl, Br, and I. More preferably, the donor impurities may be Al, Ga, or In. Alternatively, the impurities doped into the hole transport enhancing layer 230 may include one or more acceptor impurities and one or more donor impurities. These impurities are doped into the hole transport enhancing layer 230 at a concentration equal to or greater than a predetermined concentration.
當上述雜質以預設濃度摻雜到電洞傳輸率提高層230中時,上述雜質可以透過利用等離子體對內部壓力緩解層220的表面進行表面處理或透過離子注入製程而形成。透過離子注入製程,可以將預設濃度(如上所述)的雜質以預設厚度注入並摻雜到電洞傳輸率提高層230。 When the aforementioned impurities are doped into the hole transport efficiency enhancing layer 230 at a predetermined concentration, the impurities can be formed by treating the surface of the internal stress relief layer 220 with plasma or by an ion implantation process. The ion implantation process allows the predetermined concentration (as described above) of the impurities to be implanted into the hole transport efficiency enhancing layer 230 at a predetermined thickness.
或者,電洞傳輸率提高層230可以在內部壓力緩解層220沉積在p型包覆層210上之後在含有上述雜質分子的氣體環境中透過高溫熱處理製程或透過300℃至1000℃的快速熱處理製程形成。 Alternatively, the hole transport efficiency enhancing layer 230 can be formed by depositing the internal stress relief layer 220 on the p-type cladding layer 210 through a high-temperature heat treatment process or a rapid thermal treatment process at 300°C to 1000°C in a gas environment containing the aforementioned impurity molecules.
或者,電洞傳輸率提高層230可以在內部壓力緩解層220沉積在p型包覆層210上之後透過用含有上述雜質分子的酸或鹼溶液對內部壓力緩解層220進行表面處理來形成。 Alternatively, the hole transport efficiency enhancement layer 230 can be formed by depositing the internal stress relief layer 220 on the p-type cladding layer 210 and then surface treating the internal stress relief layer 220 with an acid or alkaline solution containing the aforementioned impurity molecules.
當p型半導體層140包括上述p型包覆層210、內部壓力緩解層220及電洞傳輸率提高層230時,能夠使在主動層130和p型包覆層210之間可能出現的內部壓力最小化,使更多的電洞傳輸到主動層130,且透過在其自身與保護層150之間形成歐姆接觸來使保護層150能夠順利地沉積。尤其,p型半導體層140可以將比以往相對大量的電洞注入到主動層130中,從而能夠去除過量 供應到主動層130中並累積在主動層130中的電子。因此,p型半導體層140可以透過去除由積累的電子在主動層130中形成的壓電電場來提高發光效率。 When p-type semiconductor layer 140 includes the aforementioned p-type cladding layer 210, internal stress relief layer 220, and hole transport efficiency enhancement layer 230, it minimizes the internal stress that may arise between active layer 130 and p-type cladding layer 210, allowing more holes to be transferred to active layer 130. Furthermore, by forming an ohmic contact between p-type semiconductor layer 140 and protective layer 150, it facilitates the deposition of protective layer 150. In particular, p-type semiconductor layer 140 can inject a significantly larger number of holes into active layer 130 than before, thereby removing electrons that are excessively supplied to and accumulated in active layer 130. Therefore, the p-type semiconductor layer 140 can improve the light emission efficiency by removing the piezoelectric field formed by the accumulated electrons in the active layer 130.
保護層150沉積在p型半導體層140上以保護p型半導體層140免受外部影響。p型半導體層140,尤其是p型半導體層140內的內部壓力緩解層220和電洞傳輸率提高層230由上述成分實現,因此與大部分的酸和鹼化學物質產生反應。因此,保護層150沉積在p型半導體層140上以保護p型半導體層140免受外部影響。另一方面,由於保護層150沉積在p型半導體層140上,因此必須在不干擾主動層130中產生的光傳播的同時擴散由電極165注入的電流,以便在p型半導體層140的整個區域內均勻地將電洞傳遞至主動層130。因此,保護層150由在可見光波長帶中的透光率等於或大於預設的第一基準值且電導率等於或大於預設的第二基準值的材料實現。例如,保護層150可以由ITO、NiO、GaZnO、InZnO、InGaZnO或石墨烯(Graphene)實現。保護層150由上述成分實現,並且透過包括電子束(E-Beam)沉積或濺射方式的物理氣相沉積(PVD:Physical Vapor Deposition)或化學氣相沉積(CVD)方法等沉積在p型半導體層140上。保護層150可以以預設厚度沉積,例如,可以以在10nm至1000nm的範圍內的厚度沉積。 Protective layer 150 is deposited on p-type semiconductor layer 140 to protect it from external influences. P-type semiconductor layer 140, particularly internal stress relief layer 220 and hole transport efficiency enhancement layer 230 within p-type semiconductor layer 140, is made of the aforementioned components and therefore reacts with most acidic and alkaline chemical substances. Therefore, protective layer 150 is deposited on p-type semiconductor layer 140 to protect it from external influences. On the other hand, because protective layer 150 is deposited on p-type semiconductor layer 140, it must diffuse the current injected by electrode 165 while undisturbed by the propagation of light generated in active layer 130, thereby uniformly transferring holes to active layer 130 across the entire region of p-type semiconductor layer 140. Therefore, protective layer 150 is implemented using a material having a transmittance in the visible light wavelength band equal to or greater than a preset first reference value and an electrical conductivity equal to or greater than a preset second reference value. For example, protective layer 150 can be implemented using ITO, NiO, GaZnO, InZnO, InGaZnO, or graphene. Protective layer 150 is formed from the aforementioned components and is deposited on p-type semiconductor layer 140 by physical vapor deposition (PVD) such as electron beam (E-beam) deposition or sputtering, or chemical vapor deposition (CVD). Protective layer 150 can be deposited to a predetermined thickness, for example, within a range of 10 nm to 1000 nm.
當以這種方式實現保護層150時,可以在保護p型半導體層140免受外部影響的同時將電洞從p型半導體層140均勻地 注入到主動層130中。 When protective layer 150 is implemented in this manner, it is possible to uniformly inject holes from p-type semiconductor layer 140 into active layer 130 while protecting p-type semiconductor layer 140 from external influences.
電極160、165分別形成在n型包覆層120和保護層150上,並向各個構成120、150供應電流。電極160形成在經過蝕刻並暴露於外部的n型包覆層120上,電極165形成在保護層150上。電極160、165可以由Al、Ag、Cr、Cu、Mo、Ni、Pd、Ti及W中的一種以上的金屬或其合金實現。尤其,由於電極165在光從主動層130照射的方向上定位,因此可以由具有優異反射率的Al或Ag實現。 Electrodes 160 and 165 are formed on the n-type cladding layer 120 and the protective layer 150, respectively, and supply current to each component 120 and 150. Electrode 160 is formed on the etched and exposed portion of the n-type cladding layer 120, while electrode 165 is formed on the protective layer 150. Electrodes 160 and 165 can be made of one or more metals selected from the group consisting of Al, Ag, Cr, Cu, Mo, Ni, Pd, Ti, and W, or alloys thereof. In particular, since electrode 165 is positioned in the direction of light irradiated from the active layer 130, it can be made of Al or Ag, which have excellent reflectivity.
由於發光元件100包括上述構成,因此可以確認其具有如圖3所示的優異的量子效率(光效率)。 Since the light-emitting element 100 includes the above-described structure, it can be confirmed that it has excellent quantum efficiency (light efficiency) as shown in Figure 3.
圖3為示出根據本發明的一實施例的發光元件和現有發光元件的內量子效率的圖表。 Figure 3 is a graph showing the internal quantum efficiency of a light-emitting element according to an embodiment of the present invention and a conventional light-emitting element.
參照圖3,可以確認,與現有發光元件相比,發光元件100的內量子效率提高了30%以上。 Referring to Figure 3, it can be confirmed that the internal quantum efficiency of light-emitting element 100 is improved by more than 30% compared to conventional light-emitting elements.
圖5至圖10為示出根據本發明的一實施例的發光元件的製造過程的圖。發光元件100的製造可以使用發光元件製造裝置來執行。 Figures 5 to 10 illustrate a process for manufacturing a light-emitting element according to an embodiment of the present invention. The light-emitting element 100 can be manufactured using a light-emitting element manufacturing apparatus.
參照圖5至圖8,在基板110上按次沉積n型包覆層120、主動層130、p型半導體層140及保護層150。 5 to 8 , an n-type cladding layer 120 , an active layer 130 , a p-type semiconductor layer 140 , and a protective layer 150 are sequentially deposited on a substrate 110 .
參照圖9,在主動層130、p型半導體層140、保護層150及n型包覆層120的一面積上進行蝕刻。蝕刻從保護層150在垂直方向上進行到n型包覆層120的一部分。 Referring to Figure 9, etching is performed on one surface of the active layer 130, the p-type semiconductor layer 140, the protective layer 150, and the n-type cladding layer 120. The etching proceeds vertically from the protective layer 150 to a portion of the n-type cladding layer 120.
參照圖10,隨著蝕刻的進行,在暴露於外部的n型包覆層120上形成電極160,且在保護層150上形成電極165。 Referring to FIG. 10 , as etching proceeds, an electrode 160 is formed on the n-type cladding layer 120 exposed to the outside, and an electrode 165 is formed on the protective layer 150 .
圖11為示出根據本發明的第二實施例的發光元件的構成的圖。 FIG11 is a diagram showing the structure of a light-emitting element according to a second embodiment of the present invention.
參照圖11,根據本發明的第二實施例的發光元件1100包括基板110、n型包覆層120、主動層1110、p型包覆層1120、保護層150及電極160、165。由於基板110、n型包覆層120、保護層150以及電極160、165與發光元件100中的構成相同,因此將省略重複的描述。 Referring to Figure 11 , a light-emitting device 1100 according to the second embodiment of the present invention includes a substrate 110, an n-type cladding layer 120, an active layer 1110, a p-type cladding layer 1120, a protective layer 150, and electrodes 160 and 165. Since the components of the substrate 110, n-type cladding layer 120, protective layer 150, and electrodes 160 and 165 are identical to those of the light-emitting device 100, repeated description will be omitted.
與主動層130同樣地,主動層1110沉積在n型包覆層120上,其中從n型包覆層120提供的電子和從p型包覆層1120提供的電洞結合以產生光。主動層130由具有相對小的能帶隙的井層(量子井,Quantum Well)和具有相對大的能帶隙的阻擋層(量子阻擋,Quantum Barrier)實現。主動層130可以由具有不同In濃度的InGaN層、InGaN/GaN或GaN/AlGaN層或它們的組合實現。 Similar to the active layer 130, the active layer 1110 is deposited on the n-type cladding layer 120, where electrons provided by the n-type cladding layer 120 combine with holes provided by the p-type cladding layer 1120 to generate light. The active layer 130 is implemented by a well layer (quantum well) with a relatively small energy bandgap and a barrier layer (quantum barrier) with a relatively large energy bandgap. The active layer 130 can be implemented by InGaN layers with different indium concentrations, InGaN/GaN, or GaN/AlGaN layers, or a combination thereof.
尤其,主動層1110在主動層1110的最外圍包括阻擋層。最外圍的阻擋層被實現為具有等於或大於預設厚度的厚度,以阻止氧氣進入主動層1110內部。然而,為了確保電子和電洞的密度和遷移率,可以實現使得n型摻雜劑摻雜到靠近n型包覆層120的最外圍阻擋層,並使得p型摻雜劑摻雜到靠近p型包覆層1120的最外圍阻擋層。透過這種方式實現,主動層1110可以防止氧氣 流入其內部。即使在主動層1110外部不包括用於防止氧流入的附加層(例如,保護層等),主動層1110也可以防止氧流入。主動層1110的具體結構如圖12和圖13所示。 In particular, active layer 1110 includes a barrier layer at its outermost periphery. This barrier layer is designed to have a thickness equal to or greater than a predetermined thickness to prevent oxygen from entering the interior of active layer 1110. However, to ensure the density and mobility of electrons and holes, n-type dopants are doped into the outermost barrier layer near n-type cladding layer 120, while p-type dopants are doped into the outermost barrier layer near p-type cladding layer 1120. This prevents oxygen from entering the active layer 1110. Even without an additional layer (e.g., a protective layer) outside the active layer 1110 for preventing oxygen inflow, the active layer 1110 can still prevent oxygen inflow. The specific structure of the active layer 1110 is shown in Figures 12 and 13.
圖12和圖13為示出根據本發明的第二實施例的主動層的構成和能帶特性的圖。 Figures 12 and 13 are diagrams showing the structure and energy band characteristics of the active layer according to the second embodiment of the present invention.
從圖12中可以確認,井層1220被實現為具有相對小的能帶隙,阻擋層1210、1230被實現為具有相對大的能帶隙。 As can be seen from FIG12 , the well layer 1220 is implemented to have a relatively small energy band gap, while the barrier layers 1210 and 1230 are implemented to have relatively large energy band gaps.
此時,如上所述,靠近n型包覆層120的最外圍阻擋層1210(在下文中稱為第一阻擋層)和靠近p型包覆層1120的最外圍阻擋層1230(在下文中稱為第二阻擋層)被實現為具有等於或大於預設厚度的厚度。此外,為了確保電子的密度和遷移率,第一阻擋層1210由以1*1016cm-3至1*1020cm-3的濃度摻雜有如Si或Ge等的GaNn型雜質的GaN、InGaN或AlGaN實現,並且,為了確保電洞的密度和遷移率,第二阻擋層1230由以1*1016cm-3至1*1020cm-3的濃度摻雜有如Mg等的p型雜質的GaN、InGaN或AlGaN實現。 At this time, as described above, the outermost barrier layer 1210 (hereinafter referred to as the first barrier layer) near the n-type cladding layer 120 and the outermost barrier layer 1230 (hereinafter referred to as the second barrier layer) near the p-type cladding layer 1120 are implemented to have a thickness equal to or greater than a preset thickness. In addition, in order to ensure the density and mobility of electrons, the first barrier layer 1210 is implemented by GaN, InGaN or AlGaN doped with GaNn-type impurities such as Si or Ge at a concentration of 1* 1016 cm -3 to 1* 1020 cm- 3 , and, in order to ensure the density and mobility of holes, the second barrier layer 1230 is implemented by GaN, InGaN or AlGaN doped with p-type impurities such as Mg at a concentration of 1* 1016 cm-3 to 1* 1020 cm -3 .
或者,如圖13所示,多個井層1220a至1220n和多個阻擋層1310a至1310n沉積在第一阻擋層1210和第二阻擋層1230之間,主動層1110可以被實現為多量子井。 Alternatively, as shown in FIG13 , multiple well layers 1220 a to 1220 n and multiple barrier layers 1310 a to 1310 n are deposited between the first barrier layer 1210 and the second barrier layer 1230 , and the active layer 1110 can be implemented as a multi-quantum well.
當主動層1110具有這種結構時,現有的基於GaN的發光元件不需要包括被包括在主動層和p型包覆層之間的電子阻擋層(Electron Blocking Layer,EBL)來控制電子的流動。 When the active layer 1110 has this structure, existing GaN-based light-emitting devices do not need to include an electron blocking layer (EBL) between the active layer and the p-type cladding layer to control the flow of electrons.
再次參照圖11,p型包覆層1120沉積在主動層1110上,尤其,第二阻擋層1230上,並向主動層1110提供電洞。此時,由於p型包覆層1120被實現為具有如圖14所示的結構,因此可以使內部壓力(應變)最小化,並提高向主動層1110的電洞的傳輸率。 Referring again to FIG. 11 , p-type cladding layer 1120 is deposited on active layer 1110, particularly on second blocking layer 1230, and provides holes to active layer 1110. Since p-type cladding layer 1120 has the structure shown in FIG. 14 , internal stress (strain) is minimized and the transmission rate of holes to active layer 1110 is improved.
圖14為示出根據本發明的第二實施例的p型包覆層的構成的圖。 FIG14 is a diagram showing the structure of a p-type cladding layer according to the second embodiment of the present invention.
參照圖14,根據本發明的第二實施例的p型包覆層1120包括內部壓力緩解層1410和電洞傳輸率提高層1420。 14 , the p-type cladding layer 1120 according to the second embodiment of the present invention includes an internal stress relief layer 1410 and a hole transport efficiency enhancement layer 1420.
除了其沉積在第二阻擋層1230的正上端上之外,內部壓力緩解層1410具有與內部壓力緩解層220相同的特性。 The internal pressure relief layer 1410 has the same properties as the internal pressure relief layer 220, except that it is deposited directly on the upper end of the second barrier layer 1230.
電洞傳輸率提高層1420也具有與電洞傳輸率提高層230相同的特性。 The hole transport efficiency enhancing layer 1420 also has the same characteristics as the hole transport efficiency enhancing layer 230.
當p型包覆層1120包括上述構成即內部壓力緩解層1410和電洞傳輸率提高層1420時,能夠使在主動層1110和其自身之間可能出現的內部壓力最小化,顯著提高電洞傳輸率,且透過在其自身與保護層150之間形成歐姆接觸來使保護層150沉積。 When p-type cladding layer 1120 includes the aforementioned components, namely internal stress relief layer 1410 and hole transport efficiency enhancement layer 1420, it can minimize the internal stress that may arise between active layer 1110 and itself, significantly improving hole transport efficiency. Furthermore, it forms ohmic contact between itself and protective layer 150, enabling deposition of protective layer 150.
可以確認由於發光元件1100包括上述構成而具有如圖18所示的發光強度的特徵。 It can be confirmed that the light-emitting element 1100 has the characteristics of light emission intensity shown in Figure 18 due to the above-mentioned structure.
圖18為示出根據本發明的第二實施例的發光元件的根據施加電流的發光強度變化的圖。 FIG18 is a graph showing changes in the light-emitting intensity of a light-emitting element according to the second embodiment of the present invention depending on the applied current.
參照圖18,可以確認發光元件1100輸出藍色波長帶中的 光,發光強度也隨著注入電流量的增加而增加。 Referring to Figure 18 , it can be confirmed that light-emitting element 1100 outputs light in the blue wavelength band, and the luminous intensity increases with increasing injected current.
圖15至圖17為示出根據本發明的第二實施例的發光元件的製造過程的圖。 Figures 15 to 17 are diagrams illustrating the manufacturing process of a light-emitting element according to the second embodiment of the present invention.
參照圖15至圖17,在基板110上按次沉積n型包覆層120、主動層130、p型半導體層140及保護層150。更具體地,內部壓力緩解層1410和電洞傳輸率提高層1420沉積在主動層130上。 15 to 17 , an n-type cladding layer 120 , an active layer 130 , a p-type semiconductor layer 140 , and a protective layer 150 are sequentially deposited on a substrate 110 . More specifically, an internal stress relief layer 1410 and a hole transport efficiency enhancement layer 1420 are deposited on the active layer 130 .
此後,根據與上面參照圖9和圖10說明的過程相同的過程製造發光元件。 Thereafter, the light-emitting element is manufactured according to the same process as that described above with reference to Figures 9 and 10.
圖19為示出根據本發明的第三實施例的發光元件的構成的圖。 FIG19 is a diagram showing the structure of a light-emitting element according to a third embodiment of the present invention.
參照圖19,根據本發明的一實施例的發光元件1900包括基板110、n型包覆層120、主動層130、p型半導體層140、電極150、155及絕緣膜1910。由於根據本發明的一實施例的發光元件1900中的基板110、n型包覆層120、主動層130及電極150、155與發光元件100中的構成相同,因此將省略重複的描述。另一方面,根據本發明的一實施例的發光元件1900中的p型半導體層140以與發光元件100中的p型半導體層相同的構成實現,除了電洞傳輸率提高層230為了在內部壓力緩解層220和電極150之間形成歐姆接觸而摻雜預設濃度的雜質之外,其餘均以相同的方式實現。 19 , a light-emitting device 1900 according to one embodiment of the present invention includes a substrate 110, an n-type cladding layer 120, an active layer 130, a p-type semiconductor layer 140, electrodes 150 and 155, and an insulating film 1910. Since the substrate 110, n-type cladding layer 120, active layer 130, and electrodes 150 and 155 in light-emitting device 1900 according to one embodiment of the present invention are identical to those in light-emitting device 100, repeated descriptions will be omitted. On the other hand, the p-type semiconductor layer 140 in the light-emitting device 1900 according to one embodiment of the present invention is implemented with the same configuration as the p-type semiconductor layer in the light-emitting device 100. Except for the hole transport efficiency enhancement layer 230 being doped with a predetermined concentration of impurities to form an ohmic contact between the internal stress relief layer 220 and the electrode 150, all other aspects are implemented in the same manner.
電極150沉積在p型半導體層140上,更具體地,沉積 在電洞傳輸率提高層230上,以向p型半導體層140供應電流。電極150由具有優良反射率的金屬實現,並將主動層130中產生的光向n型包覆層120反射。通常,電極150可以透過使用電子束(Electron Beam,EB)法、蒸發法或濺射法等方法沉積形成。電極150具有如圖20a或圖20b所示的構成並執行上述的操作。 Electrode 150 is deposited on p-type semiconductor layer 140, more specifically, on hole transport efficiency enhancing layer 230, to supply current to p-type semiconductor layer 140. Electrode 150 is made of a metal with excellent reflectivity and reflects light generated in active layer 130 toward n-type cladding layer 120. Typically, electrode 150 can be deposited using methods such as electron beam (EB), evaporation, or sputtering. Electrode 150 has the structure shown in Figure 20a or Figure 20b and performs the above-described operations.
圖20a及圖20b為示出根據本發明的第三實施例的電極層的構成的圖。 Figures 20a and 20b are diagrams showing the structure of an electrode layer according to the third embodiment of the present invention.
參照圖20a,根據本發明的一實施例的電極層150(下面將描述的155也相同)包括金屬電極2010和保護層2020。 Referring to FIG. 20a , the electrode layer 150 (the same also applies to 155 described below) according to one embodiment of the present invention includes a metal electrode 2010 and a protective layer 2020.
金屬電極2010在起到電極作用的同時反射入射到其上的光。金屬電極2010沉積在電洞傳輸率提高層230上並將向其入射的光反射。金屬電極2010可以由鋁(Al)實現或可以包括鋁(Al)和銀(Ag)。當由鋁實現時,金屬電極2010可以被實現為具有20nm至10,000nm的厚度。當包括鋁和銀時,金屬電極2010可以透過首先沉積厚度小於10nm的鋁,然後在鋁上沉積厚度為200nm至1,000nm的銀來實現。 The metal electrode 2010 functions as an electrode while reflecting incident light. The metal electrode 2010 is deposited on the hole transport efficiency enhancing layer 230 and reflects incident light. The metal electrode 2010 can be made of aluminum (Al) or can include aluminum (Al) and silver (Ag). When made of aluminum, the metal electrode 2010 can have a thickness of 20 nm to 10,000 nm. When including aluminum and silver, the metal electrode 2010 can be formed by first depositing aluminum to a thickness of less than 10 nm and then depositing silver to a thickness of 200 nm to 1,000 nm on the aluminum.
保護層2020沉積在金屬電極2010上以保護金屬電極2010免受外部影響。如上所述,金屬電極2010由具有優異反射率的金屬即鋁或銀實現,以反射入射到其上的光。然而,實現金屬電極2010的金屬容易被氧化且具有容易與水或其他化學物質發生化學反應的性質。因此,保護層2020沉積在金屬電極2010上以使金屬電極2010暴露於外部環境最小化。保護層2020可以由與其 他成分的反應性低的鋁(Al)、鈦(Ti)、鉻(Cr)、鎳(Ni)、銅(Cu)、鈀(Pd)、鉬(Mo)、鉭(Ta)、鎢(W)、錸(Re)、鉑(Pt)、金(Au)或上述成分的合金實現。 A protective layer 2020 is deposited on the metal electrode 2010 to protect it from external influences. As mentioned above, the metal electrode 2010 is made of a metal with excellent reflectivity, such as aluminum or silver, to reflect incident light. However, the metal used to make the metal electrode 2010 is easily oxidized and reacts chemically with water and other chemicals. Therefore, the protective layer 2020 is deposited on the metal electrode 2010 to minimize its exposure to the external environment. The protective layer 2020 can be made of aluminum (Al), titanium (Ti), chromium (Cr), nickel (Ni), copper (Cu), palladium (Pd), molybdenum (Mo), tungsten (W), ruthenium (Re), platinum (Pt), gold (Au), or alloys thereof, which have low reactivity with other components.
當電極層150具有這種結構時,其可以將電流傳輸到p型半導體層140並反射入射到其上的光,同時具有高穩定性。 When the electrode layer 150 has this structure, it can transmit current to the p-type semiconductor layer 140 and reflect light incident thereon while having high stability.
另一方面,根據本發明的一實施例的電極層150可以如圖20b所示實現。 On the other hand, the electrode layer 150 according to one embodiment of the present invention can be implemented as shown in FIG. 20b.
參照圖20b,根據本發明的一實施例的電極層150(下面將描述的155也相同)除了金屬電極2010和保護層2020之外還可包括金屬接觸層2030。 Referring to FIG. 20 b , the electrode layer 150 (the same also applies to 155 described below) according to one embodiment of the present invention may include a metal contact layer 2030 in addition to the metal electrode 2010 and the protective layer 2020.
即使金屬電極2010沉積在電洞傳輸率提高層230上,也由於其相對弱的接觸力而存在容易剝離的可能性。因此,為了在電洞傳輸率提高層230上提高金屬電極2010的接觸力,金屬接觸層2030可以優先沉積在上述電洞傳輸率提高層230和金屬電極2010之間。金屬接觸層2030可以由鋁(Al)實現,且可以以厚度小於10nm的薄膜的形式沉積。或者,為了進一步提高接觸力,金屬接觸層2030可以以由鉻(Cr)、鈦(Ti)、鈀(Pd)或鉬(Mo)實現的附加金屬層以小於2nm的厚度首先沉積在電洞傳輸率提高層230上後在該層上沉積厚度小於10nm的鋁(Al)層的形式實現。金屬電極2010和保護層2020可以沉積在金屬接觸層2030上,從而可以進一步提高金屬電極2010和保護層2020的接觸力。 Even if the metal electrode 2010 is deposited on the hole transport efficiency enhancing layer 230, it may be easily peeled off due to its relatively weak contact force. Therefore, in order to improve the contact force of the metal electrode 2010 on the hole transport efficiency enhancing layer 230, the metal contact layer 2030 can be preferentially deposited between the hole transport efficiency enhancing layer 230 and the metal electrode 2010. The metal contact layer 2030 can be implemented by aluminum (Al) and can be deposited in the form of a thin film with a thickness of less than 10 nm. Alternatively, to further enhance contact strength, the metal contact layer 2030 can be implemented by first depositing an additional metal layer made of chromium (Cr), titanium (Ti), palladium (Pd), or molybdenum (Mo) with a thickness of less than 2 nm on the hole transport efficiency enhancing layer 230, followed by depositing an aluminum (Al) layer with a thickness of less than 10 nm on this layer. The metal electrode 2010 and the protective layer 2020 can be deposited on the metal contact layer 2030, thereby further enhancing the contact strength between the metal electrode 2010 and the protective layer 2020.
再次參照圖19,電極150具有上述結構並執行上述操作。 此時,電極150沉積在p型半導體層140上時可以具有如圖23或圖24所示的結構。 Referring again to FIG. 19 , electrode 150 has the structure described above and performs the above-described operations. At this point, electrode 150, when deposited on p-type semiconductor layer 140, may have the structure shown in FIG. 23 or FIG. 24 .
圖23和圖24為示出根據本發明的第三實施例的電極的結構的圖。 Figures 23 and 24 are diagrams showing the structure of an electrode according to a third embodiment of the present invention.
參照圖23,根據本發明的一實施例的電極150可以具有均勻沉積在p型半導體層140上的結構,更具體地,均勻沉積在電洞傳輸率提高層230上的結構。 23 , the electrode 150 according to one embodiment of the present invention may have a structure uniformly deposited on the p-type semiconductor layer 140 , more specifically, a structure uniformly deposited on the hole transport efficiency enhancing layer 230 .
另一方面,參照圖24,在沉積電極150之前,可以對內部壓力緩解層220和電洞傳輸率提高層230的一部分或以預設的間隔進行蝕刻。因此,p型包覆層210的一部分可以被暴露。可以在對內部壓力緩解層220和電洞傳輸率提高層230進行蝕刻的狀態下進行電極150的沉積。因此,電極150可以直接接觸p型包覆層210的一部分,因此不需要穿過內部壓力緩解層220和電洞傳輸率提高層230,能夠直接更有效地向p型包覆層210傳輸電流。 On the other hand, referring to FIG. 24 , before depositing the electrode 150, a portion of the internal stress-relieving layer 220 and the hole-transport-enhancing layer 230 can be etched, or at predetermined intervals. This exposes a portion of the p-type cladding layer 210. The electrode 150 can be deposited while the internal stress-relieving layer 220 and the hole-transport-enhancing layer 230 are being etched. This allows the electrode 150 to directly contact a portion of the p-type cladding layer 210, eliminating the need for the electrode 150 to pass through the internal stress-relieving layer 220 and the hole-transport-enhancing layer 230. This allows for more efficient current transfer directly to the p-type cladding layer 210.
再次參照圖19,電極155沉積在n型包覆層120上,以向n型包覆層120供應電子。通常,電極155可以透過使用電子束(EB)法、蒸發法或濺射法等方法沉積形成。同樣地,電極155也與電極150一樣由具有優異反射率的金屬實現,從而提高光提取效率。在結構上,主動層130中產生的光不會直接到達電極155。然而,由於發光元件100和空氣之間的折射率差異,主動層130中產生的光被捕獲在發光元件100內。因此,從主動層130產生並 釋放的大量光也可以被入射到電極155。電極155由具有優異反射率的金屬實現,透過反射光而不是吸收光來改善發光元件100的光輸出特性。 Referring again to Figure 19 , electrode 155 is deposited on n-type cladding layer 120 to supply electrons to n-type cladding layer 120. Typically, electrode 155 can be deposited using methods such as electron beam (EB) deposition, evaporation, or sputtering. Like electrode 150, electrode 155 is made of a metal with excellent reflectivity, thereby improving light extraction efficiency. Structurally, light generated in active layer 130 does not directly reach electrode 155. However, due to the refractive index difference between light-emitting element 100 and air, light generated in active layer 130 is trapped within light-emitting element 100. Therefore, a significant amount of light generated and released from active layer 130 can also be incident on electrode 155. Electrode 155 is made of a metal with excellent reflectivity, improving the light output characteristics of light-emitting element 100 by reflecting light rather than absorbing it.
如圖20a所示,電極155包括上述的反射電極2010和保護層2020,或者如圖20b所示,電極155除了金屬電極2010和保護層2020之外還可包括金屬接觸層2030。因此,電極155具有如圖21或22所示的電特性。 As shown in FIG20a, electrode 155 includes the aforementioned reflective electrode 2010 and protective layer 2020. Alternatively, as shown in FIG20b, electrode 155 may include a metal contact layer 2030 in addition to metal electrode 2010 and protective layer 2020. Therefore, electrode 155 has the electrical characteristics shown in FIG21 or FIG22.
圖21為示出由不同成分實現的電極的電壓和電流特性的圖表,圖22a及圖22b為示出Al或Al/Ag基歐姆電極的電壓和電流特性的圖表。 Figure 21 is a graph showing the voltage and current characteristics of electrodes realized with different compositions, and Figures 22a and 22b are graphs showing the voltage and current characteristics of Al or Al/Ag-based ohmic electrodes.
參照圖21,可以確認,即使包含鋁(Al)或鋁(Al)和銀(Ag)的金屬電極2010優先沉積在n型包覆層120上,也可以形成高品質的歐姆接觸。然而,若首先沉積由鉻(Cr)等實現的金屬接觸層2030,然後沉積金屬電極2010,則可以獲得更穩定的接觸力,且能夠形成高品質的歐姆接觸。 Referring to Figure 21 , it can be confirmed that even when the metal electrode 2010 comprising aluminum (Al) or aluminum (Al) and silver (Ag) is preferentially deposited on the n-type cladding layer 120, a high-quality ohmic contact can be formed. However, if a metal contact layer 2030 made of, for example, chromium (Cr) is first deposited, followed by the metal electrode 2010, a more stable contact is achieved, enabling the formation of a high-quality ohmic contact.
另一方面,參照圖22a及圖22b,雖然銀(Ag)是具有最高反射率的金屬,但是當沉積在n型包覆層120上時,不形成歐姆接觸,因此將其用作n型金屬電極2010可能存在困難。然而,如上所述,由於金屬電極2010被實現為包括鋁和銀,因此其可以形成高品質的歐姆接觸。另外,可以在兩者即電洞傳輸率提高層230和n型金屬電極2010之間額外沉積金屬接觸層2030,以形成更優異的歐姆接觸。因此,電極150、155可以與p型半導體層140 形成優異的歐姆接觸。 On the other hand, referring to Figures 22a and 22b, although silver (Ag) has the highest reflectivity, it does not form an ohmic contact when deposited on n-type cladding layer 120, making its use as n-type metal electrode 2010 potentially challenging. However, as described above, since metal electrode 2010 is implemented as comprising aluminum and silver, it can form a high-quality ohmic contact. Furthermore, metal contact layer 2030 can be additionally deposited between hole transport efficiency enhancing layer 230 and n-type metal electrode 2010 to form an even better ohmic contact. Consequently, electrodes 150 and 155 can form an excellent ohmic contact with p-type semiconductor layer 140.
再次參照圖19,絕緣膜1910層疊到n型包覆層120、主動層130及p型半導體層140的側面和電極150、155的側面和上面的一部分,從而保護發光元件100內的每個構成免受外部影響,且將n型區域和p型區域電隔離。 Referring again to Figure 19 , an insulating film 1910 is laminated onto the side surfaces of the n-type cladding layer 120 , the active layer 130 , and the p-type semiconductor layer 140 , as well as the side surfaces and a portion of the top surface of the electrodes 150 and 155 , thereby protecting each component within the light-emitting element 100 from external influences and electrically isolating the n-type region from the p-type region.
圖25和圖26為示出根據本發明的第三實施例的發光元件的製造過程的圖。 Figures 25 and 26 are diagrams illustrating the manufacturing process of a light-emitting element according to the third embodiment of the present invention.
進行如圖5至圖9所示的製造過程。 The manufacturing process is carried out as shown in Figures 5 to 9.
參照圖25,在進行蝕刻的同時,在暴露於外部的n型包覆層120上沉積電極155。 Referring to FIG. 25 , while etching is being performed, an electrode 155 is deposited on the n-type cladding layer 120 exposed to the outside.
參照圖26,絕緣膜1910層疊到n型包覆層120、主動層130及p型半導體層140的側面及電極150、155的側面和上面的一部分。 Referring to Figure 26, the insulating film 1910 is laminated onto the side surfaces of the n-type cladding layer 120, the active layer 130, and the p-type semiconductor layer 140, as well as the side surfaces and a portion of the top surface of the electrodes 150 and 155.
圖27為示出根據本發明的第四實施例的發光元件的構成的圖。 FIG27 is a diagram showing the structure of a light-emitting element according to a fourth embodiment of the present invention.
參照圖27,根據本發明的第四實施例的發光元件2700包括基板2710、n型包覆層2720、主動層2730、p型半導體層2740、透明電極2750及電極2760、2765。基板2710、n型包覆層2720及主動層2730以與基板110、n型包覆層120及主動層130相同的構成實現,並且能夠執行相同的操作。 Referring to Figure 27 , a light-emitting device 2700 according to the fourth embodiment of the present invention includes a substrate 2710, an n-type cladding layer 2720, an active layer 2730, a p-type semiconductor layer 2740, a transparent electrode 2750, and electrodes 2760 and 2765. Substrate 2710, n-type cladding layer 2720, and active layer 2730 have the same configuration as substrate 110, n-type cladding layer 120, and active layer 130, and can perform the same operations.
p型半導體層2740沉積在主動層2730上並向主動層2730提供電洞。此時,由於p型半導體層2740採用如圖28所示的結 構來實現,因此透過防止光輸出到在光輸出方向上佈置的電極2765(在遠離基板2710的位置佈置的電極),可以提高發光元件2700的光輸出。 A p-type semiconductor layer 2740 is deposited on the active layer 2730 and provides holes to the active layer 2730. Since the p-type semiconductor layer 2740 employs the structure shown in Figure 28 , it prevents light from being emitted to the electrode 2765 located in the light emission direction (the electrode located away from the substrate 2710), thereby improving the light output of the light-emitting element 2700.
圖28為示出根據本發明的第四或第五實施例的p型半導體層的構成的圖,圖29為根據本發明的第四或第五實施例的p型半導體層的平面圖,圖30為比較根據本發明的第四實施例的發光元件和現有發光元件的光效率的圖。 FIG28 is a diagram illustrating the configuration of a p-type semiconductor layer according to the fourth or fifth embodiment of the present invention. FIG29 is a plan view of the p-type semiconductor layer according to the fourth or fifth embodiment of the present invention. FIG30 is a graph comparing the light emitting element according to the fourth embodiment of the present invention and a conventional light emitting element.
參照圖28,根據本發明的第四或第五實施例的p型半導體層2740包括p型包覆層2810和p型氧化物層2820。p型包覆層2810和p型氧化物層2820分別以與p型包覆層210和內部壓力緩解層220相同的構成實現,並且能夠執行相同的操作。 28 , the p-type semiconductor layer 2740 according to the fourth or fifth embodiment of the present invention includes a p-type cladding layer 2810 and a p-type oxide layer 2820. The p-type cladding layer 2810 and the p-type oxide layer 2820 are implemented with the same configurations as the p-type cladding layer 210 and the internal stress relief layer 220, respectively, and are capable of performing the same operations.
另一方面,面積等於或大於電極2765的面積的電流流動阻礙部2830形成在p型包覆層2810內的一個區域,更具體地,形成在將要佈置電極2765的區域的垂直下方。電流流動阻礙部2830透過使用氧氣或含氧氣體的等離子體處理或離子/電子注入製程來形成。相關製程在與p型包覆層2810上的電極2765的中心一致的位置處進行,且覆蓋等於或大於電極2765的總(截)面積的面積。當在p型包覆層2810中執行等離子體處理或離子/電子注入製程時,由於上述的處理,p型包覆層2810的物理特性(主要是影響電流流動或電特性的特性)發生變化,以阻礙電流(電洞)的流動。在已執行等離子體處理或注入製程的區域中,電流(此處為電洞)的流動受到阻礙。此後,在物理特性發生變化的p型包覆 層2810上沉積p型氧化物層2820時,構成p型氧化物層2820的成分會影響p型包覆層2810的物理特性變化的區域,完成p型包覆層2810內的電流流動阻礙部2830。這可以在圖29中清楚地確認。參照圖29,可以確認,當p型氧化物層2820沉積在p型包覆層2810上時,電流流動阻礙部2830形成在兩者即p型包覆層2810和p型氧化物層2820之間的邊界處。電流流動阻礙部2830阻擋大部分電流或完全阻擋電流。由於電流流動阻礙部2830不是透過在p型包覆層2810上添加單獨的薄膜層來實現的,因此不需要額外的沉積製程。 On the other hand, a current flow barrier 2830, having an area equal to or greater than that of electrode 2765, is formed in a region within p-type cladding layer 2810, more specifically, vertically below the region where electrode 2765 will be positioned. Current flow barrier 2830 is formed by plasma treatment or ion/electron implantation using oxygen or an oxygen-containing gas. This process is performed at a location aligned with the center of electrode 2765 on p-type cladding layer 2810, and covers an area equal to or greater than the total (cross-sectional) area of electrode 2765. When plasma treatment or ion/electron implantation is performed on p-type cladding layer 2810, the physical properties (primarily those that affect current flow or electrical characteristics) of p-type cladding layer 2810 change, hindering the flow of current (holes). The flow of current (in this case, holes) is hindered in the areas where the plasma treatment or implantation process has occurred. Subsequently, when p-type oxide layer 2820 is deposited on p-type cladding layer 2810 with altered physical properties, the composition of p-type oxide layer 2820 influences the areas where the physical properties of p-type cladding layer 2810 have changed, thereby forming current flow blocking portion 2830 within p-type cladding layer 2810. This can be clearly seen in Figure 29 . Referring to Figure 29 , it can be seen that when p-type oxide layer 2820 is deposited on p-type cladding layer 2810, current flow block 2830 is formed at the boundary between p-type cladding layer 2810 and p-type oxide layer 2820. Current flow block 2830 blocks most or all current. Since current flow block 2830 is not implemented by adding a separate thin film layer on p-type cladding layer 2810, no additional deposition process is required.
由於電流流動阻礙部2830形成在電極2765的垂直下方,且其面積至少等於電極2765的面積,因此,當p型包覆層2810將電洞傳輸到主動層2730時,將電洞傳輸到除了形成有電流流動阻礙部2830的區域之外的其他所有區域的主動層2730。因此,當電洞和電子在主動層2730中複合並發射光時,在除電極2765所在的部位之外的區域中產生的光可以在不受到電極2765的顯著干擾的情況下自由地逸出主動層2730。從圖30中可以確認,發光元件2700的光輸出與現有發光元件相比提高了約7%。 Because the current flow barrier 2830 is formed vertically below the electrode 2765 and its area is at least equal to the area of the electrode 2765, when the p-type cladding layer 2810 transfers holes to the active layer 2730, the holes are transferred to all areas of the active layer 2730 except the area where the current flow barrier 2830 is formed. Therefore, when holes and electrons recombine in the active layer 2730 and emit light, the light generated in areas other than the area where the electrode 2765 is located can freely escape the active layer 2730 without being significantly disturbed by the electrode 2765. As shown in Figure 30, the light output of the light-emitting element 2700 is increased by approximately 7% compared to conventional light-emitting elements.
再次參照圖27,透明電極2750堆疊在p型半導體層2740上,更具體地,堆疊在p型氧化物層2820上,並向p型半導體層2740供應電流。為了將電流(電洞)從p型半導體層2740供應到主動層2730的除了電流流動阻礙部2830之外的整個區域,具有優良導電率和良好透明度的透明電極2750被沉積在p型氧化物層 2820上。透明電極2750可以由ITO、NiO、GaZnO、InZnO或InGaZnO實現,以具有透明性和優異的導電率。 Referring again to Figure 27 , transparent electrode 2750 is stacked on p-type semiconductor layer 2740, more specifically, on p-type oxide layer 2820, and supplies current to p-type semiconductor layer 2740. To supply current (holes) from p-type semiconductor layer 2740 to the entire area of active layer 2730, excluding current flow blocking portion 2830, transparent electrode 2750, which exhibits excellent conductivity and good transparency, is deposited on p-type oxide layer 2820. Transparent electrode 2750 can be made of ITO, NiO, GaZnO, InZnO, or InGaZnO, due to their transparency and excellent conductivity.
電極2760、2765分別形成在n型包覆層2720和透明電極2750上,並向各個構成2720、2750供應電流。電極2760形成在經過蝕刻並暴露於外部的n型包覆層2720上,電極2765形成在透明電極2750上。電極2760、2765可以由Al、Ag、Cr、Cu、Mo、Ni、Pd、Ti及W中的一種以上的金屬或其合金實現。 Electrodes 2760 and 2765 are formed on n-type cladding layer 2720 and transparent electrode 2750, respectively, and supply current to each component 2720 and 2750. Electrode 2760 is formed on the etched and exposed portion of n-type cladding layer 2720, while electrode 2765 is formed on transparent electrode 2750. Electrodes 2760 and 2765 can be made of one or more metals selected from the group consisting of Al, Ag, Cr, Cu, Mo, Ni, Pd, Ti, and W, or alloys thereof.
由於發光元件2700包括上述構成,因此可以透過最小化照射到電極2765的光來確保優異的光輸出。 Since light-emitting element 2700 includes the above-described structure, it is possible to ensure excellent light output by minimizing the amount of light that strikes electrode 2765.
圖31至圖37為示出根據本發明的第四實施例的發光元件的製造過程的圖。發光元件2700的製造可以使用發光元件製造裝置來執行。 Figures 31 to 37 illustrate a process for manufacturing a light-emitting element according to a fourth embodiment of the present invention. Light-emitting element 2700 can be manufactured using a light-emitting element manufacturing apparatus.
參照圖31及圖32,在基板2710上按次沉積n型包覆層2720、主動層2730及p型包覆層2810。 31 and 32 , an n-type cladding layer 2720 , an active layer 2730 , and a p-type cladding layer 2810 are sequentially deposited on a substrate 2710 .
參照圖33,在沉積p型包覆層2810之後,對要形成電流流動阻礙部2830的區域(至少在電極2765的垂直下方的相同區域)進行等離子體處理或離子/電子注入製程。 Referring to FIG. 33 , after depositing the p-type cladding layer 2810, a plasma treatment or ion/electron implantation process is performed on the region where the current flow barrier 2830 is to be formed (at least the same region vertically below the electrode 2765).
參照圖34,p型氧化物層2820沉積在p型包覆層2810上。因此,電流流動阻礙部2830形成在p型包覆層2810內。 Referring to FIG. 34 , a p-type oxide layer 2820 is deposited on a p-type cladding layer 2810 . Thus, a current flow barrier 2830 is formed within the p-type cladding layer 2810 .
參照圖35,透明電極2750堆疊在p型氧化物層2820上。 Referring to Figure 35, the transparent electrode 2750 is stacked on the p-type oxide layer 2820.
參照圖36,從透明電極2750到n型包覆層2720的某一位置以檯面結構的形式進行蝕刻。 Referring to Figure 36, etching is performed from the transparent electrode 2750 to a certain position of the n-type cladding layer 2720 in the form of a countertop structure.
參照圖37,隨著蝕刻的進行,在暴露於外部的n型包覆層2720上形成電極2760,且在透明電極2750上形成電極2765。 Referring to FIG. 37 , as etching proceeds, an electrode 2760 is formed on the n-type cladding layer 2720 exposed to the outside, and an electrode 2765 is formed on the transparent electrode 2750.
圖38為示出根據本發明的第五實施例的發光元件的構成的圖。 FIG38 is a diagram showing the structure of a light-emitting element according to a fifth embodiment of the present invention.
參照圖38,根據本發明的第五實施例的發光元件3800在p型包覆層2810內還可包括漏電流防止部3810。 38 , the light-emitting element 3800 according to the fifth embodiment of the present invention may further include a leakage current prevention portion 3810 within the p-type cladding layer 2810.
發光元件3800中的p型包覆層2810在兩末端還可包括漏電流防止部3810。若發光元件具有檯面結構,則可能出現不期望的電流被注入到檯面邊緣處的p型包覆層2810等中的問題。 The p-type cladding layer 2810 in the light-emitting element 3800 may also include leakage current prevention portions 3810 at both ends. If the light-emitting element has a countertop structure, there is a risk of undesired current being injected into the p-type cladding layer 2810 at the countertop edge.
為了防止上述問題,p型包覆層2810在兩末端還可包括漏電流防止部3810。如上面參照圖36所述,當以檯面結構的形式從透明電極2750到n型包覆層2720的某一位置進行蝕刻,且p型包覆層2810的側面暴露於外部時,可以額外使用氧氣或含氧氣體進行附加等離子體處理。即使進行等離子體處理,p型氧化物層2820的物理特性(主要是影響電流流動或電特性的特性)也不會改變,僅p型包覆層2810的物理特性改變。因此,由於沉積有p型氧化物層2820而未完全暴露於外部的p型包覆層2810的區域不發生物理特性的變化,但已蝕刻並暴露於外部的側面(末端)及從其預設的面積範圍內發生物理特性變化。透過上述過程,從p型包覆層2810的兩末端開始的預設面積的區域被實現為漏電流防止部3810,與電流流動阻礙部2830同樣地,阻礙電流的流動。 To prevent this problem, p-type cladding layer 2810 may further include leakage current prevention portions 3810 at both ends. As described above with reference to FIG. 36 , when etching is performed from transparent electrode 2750 to a certain location on n-type cladding layer 2720 in a planar structure, and the side surfaces of p-type cladding layer 2810 are exposed to the outside, an additional plasma treatment using oxygen or an oxygen-containing gas may be performed. Even with this plasma treatment, the physical properties of p-type oxide layer 2820 (primarily those that affect current flow and electrical characteristics) remain unchanged; only the physical properties of p-type cladding layer 2810 are altered. Therefore, the areas of p-type cladding layer 2810 not fully exposed due to the deposition of p-type oxide layer 2820 do not experience changes in physical properties. However, the etched and exposed sides (ends) and the area extending beyond the predetermined area do experience changes in physical properties. Through this process, the predetermined area extending from both ends of p-type cladding layer 2810 becomes leakage current prevention portion 3810, which, like current flow blocking portion 2830, blocks the flow of current.
p型包覆層2810可以另外包括漏電流防止部3810以阻 止在兩末端產生漏電流,從而進一步提高發光元件3800的光輸出。 The p-type cladding layer 2810 may further include a leakage current prevention portion 3810 to prevent leakage current from occurring at both ends, thereby further improving the light output of the light-emitting element 3800.
以上說明僅僅是本實施例的技術思想的示例性說明,本領域技術人員可以在不背離本發明的本質特徵的情況下進行各種修改和變型。因此,提供本實施例不是僅為了限制,而是為了解釋本實施例的技術思想,並且本實施例的技術思想的範圍不限於這些實施例。本實施例的保護範圍應該透過所附請求項所解釋,以及在等效範圍內所有技術精神應該被解釋為包括在本實施例的專利權範圍中。 The above description is merely an illustrative illustration of the technical concept of this embodiment. Those skilled in the art may make various modifications and variations without departing from the essential characteristics of the present invention. Therefore, the present embodiment is provided not merely for limitation but for explanation of the technical concept of this embodiment, and the scope of the technical concept of this embodiment is not limited to these embodiments. The scope of protection of this embodiment should be interpreted by the appended claims, and all technical spirit within the scope of equivalents should be interpreted as being included within the scope of patent rights of this embodiment.
100:發光元件 100: Light-emitting element
110:基板 110:Substrate
120:n型包覆層 120: n-type cladding layer
130:主動層 130: Active layer
140:p型半導體層 140: p-type semiconductor layer
150:保護層 150: Protective layer
160、165:電極 160, 165: Electrode
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